[0001] The present invention is concerned in general with circuit arrangements which alter
the dynamic range of audio signals, namely compressors which compress the dynamic
range and expanders which expand the dynamic range. More particularly, the invention
relates to improvements in transient control aspects of circuit arrangements for altering
the dynamic range of audio signals.
[0002] Compressors and expanders are normally used together (a compander system) to effect
noise reduction; the signal is compressed before transmission or recording and expanded
after reception or playback from the transmission channel. However, compressors may
be used alone to reduce the dynamic range, e.g., to suit the capacity of a transmission
channel, without subsequent expansion when the compressed signal is adequate for the
end purpose. In addition, compressors alone are used in certain products, especially
audio products which are intended only to transmit or record compressed broadcast
or pre-recorded signals. Expanders alone are used in certain products, especially
audio products which are intended only to receive or play back already compressed
broadcast or pre-recorded signals. In certain products, a single device is often configured
for switchable mode operation as a compressor to record signals and as an expander
to play back compressed broadcast or pre-recorded signals.
[0003] A dominant signal component is a signal component having a substantial enough level
so as to effect dynamic action within the frequency band under consideration. Under
complex signal conditions there may be more than one dominant signal component or
a dominant signal component and sub-dominant signal components. In a compander system
which relies on complementarity of the compressor and expander, all of the signal
components must be compressed and expanded in accordance with a defined compression/expansion
law in order that the signal spectrum including the dominant signal component (and
other signals affected by dynamic action) can be restored to their correct levels
in the expander.
[0004] Sliding band circuits employ signal dependent variable filtering to provide dynamic
action. Generally, a dominant signal component causes the cutoff to turnover frequency
(or frequencies) of one or more variable filters (e.g., high pass, low pass, shelf,
notch, etc.) to shift so as to compress or expand the dominant signal component. For
example, for the case of high frequency audio compression or expansion a high frequency
boost (for compression) or cut (for expansion) can be achieved by using a high pass
filter with a variable lower corner frequency. As the signal in the high frequency
band increases, the filter corner frequency slides upwardly so as to narrow the boosted
or cut band and exclude the useful signal from the boost or cut. Such circuits can
also be configured to act at low frequencies in which case low frequency boost or
cut can be provided by way of a low pass filter with a variable upper corner frequency.
[0005] A sliding band system operating only in a single high frequency band is described
in US-PS Re 28,426 and US-PS 4,490,691. This system, which forms the basis for the
well known consumer companding type audio noise reduction system known as B-type
noise reduction, includes, in a dual path arrangement, a side path having a fixed
high pass filter in series with a variable filter.
[0006] Fixed band circuits employ variable gain or loss devices to provide dynamic action.
In fixed band circuits the compression or expansion is effected to the same degree
within the entire frequency band in which the circuit operates.
[0007] Examples of fixed band circuits are to be found in US-PS 3,846,719; 3,903,485; and
in
Journal of the Audio Engineering Society, Vol. 15, No. 4, October, 1967, pp. 383-388. In the latter reference, the well known
professional companding type audio noise reduction system known as A-type noise reduction
is described. In that system, fixed band circuits are embodied in bandsplitting arrangements
in which the frequency spectrum is split into a plurality of bands by corresponding
bandpass filters and the dynamic action is essentially independent in each frequency
band.
[0008] It is also possible to employ a single fixed band circuit operating throughout the
input signal frequency band. Such arrangements are known as wideband compressors and
expanders.
[0009] A "dual path" arrangement is one in which a compression or expansion characteristic
is achieved through the use of a main path which is essentially free of dynamic action
and one or more secondary or side paths having dynamic action. The side path or paths
take their input from the input or output of the main path and their output or outputs
are additively or subtractively combined with the main path in order to provide compression
or expansion. Generally, a side path provides a type of limiting or variable attenuation
(such as by way of a fixed band or sliding band circuit) and the manner in which it
is connected to the main path determines if it boosts (to provide compression) or
bucks (opposes) (to provide expansion) the main path signal components. Such dual
path arrangements are described in detail in US-PS 3,846,719; US-PS 3,903,485; US-PS4,490,691
and US-PS Re 28,426.
[0010] Although it is possible to configure a sliding band circuit or a fixed band circuit
using as the variable element an automatically responsive device, such as a diode
type of limiting device, it is generally preferred to employ a controlled device that
is responsive to a control signal. The latter approach gives the circuit designer
flexibility in controlling the operation of the circuit by performing operations on
the control signal (for example, frequency selective and/or level dependent amplification
of the control signal as done in the A-type and B-type systems).
[0011] In the A-type and B-type systems mentioned above, the source-drain path of field
effect transistors (FETs) are employed as voltage controlled variable resistors (forming
the variable element of a variable attenuator in the A-type system and forming the
variable element of a variable filter in the B-type system). DC control voltages,
derived from the input signals, are applied to the FET gates. The derivation includes
rectification, smoothing, and adjustment of the control voltage amplitude as necessary
to achieve the desired dynamic action. As the control voltage increases, the degree
of limiting increases: by increasing the attenuation in the fixed band circuits and,
in the sliding band circuits, by shifting the corner frequency of the filter farther
and farther from its quiescent position.
[0012] One disadvantage of the control circuit arrangement in the A-type, B-type, and other
known compander systems is that the DC control signal is formed from the linear additive
combination of the pass-band signals and the stop-band signals reaching the control
circuit. In the case of fixed band circuits in a bandsplitting system, the pass-band
is the frequency band in which a particular circuit operates; the stop-band is the
remainder of the signal spectrum handled by the system. In the case of sliding band
circuits, the pass-band is the frequency band within the pass-band of the variable
filter and the stop-band is the frequency band outside its pass-band. In an ideal
circuit, compression or expansion should not be affected by the levels of signals
outside the pass-band of the fixed band or the pass-band of the sliding band (whether
or not in its quiescent position). A solution to the problem is set forth in US-PS
4,498,055.
[0013] In accordance with the teachings in US-PS 4,498,055, the formation of the DC control
signal is altered, in a level dependent way, so as to make the DC control signal less
responsive to stop-band signal components as the level of the input signal rises.
In practical embodiments, this is accomplished by opposing (or bucking) the control
signal with a signal referred to as the modulation control signal. In the case of
a fixed band circuit, the modulation control signal assures that the amount of gain
becomes no more than necessary to assure that a dominant controlling signal is not
boosted (in the case of compression) above a reference level. In the case of a sliding
band circuit, the modulation control signal assures that the amount of frequency sliding
of the variable filter is no more than necessary to assure that a dominant controlling
signal is not boosted (in the case of compression) above a reference level. In each
case, the modulation control signal causes the DC control signal to be less than it
would be otherwise for high level signals. As a consequence, for high level input
signals, the output signals from the dynamic action circuit are higher than they would
be otherwise.
[0014] A basic design conflict in companding type noise reduction systems is the requirement
to balance the ability to handle rapidly changing waveforms (to minimize signal overshoots)
against the desirability of minimizing signal modulation and noise modulation. The
ability of a compressor (or expander) to respond to a rapid amplitude change in its
input signal is directly related to its attack time or the time which is required
for the device to change its gain (or shift its filter corner frequency) in response
to the input amplitude change. Long attack times tend to reduce modulation distortion.
When the change in input signal amplitude occurs more abruptly than the device is
capable of changing its gain or corner frequency (caused by control circuit lag),
an overshoot results. For example, if a compressor has a gain of two times (resulting
from some steady state input condition) and suddenly the input signal doubles in amplitude
such that that compressor is unable to reduce its gain to provide the desired gain
according to its compression law, the output signal will exceed its desired amplitude
and may exceed the desired maximum output of the device, depending on the amplitude
jump and suddenness with which the input signal increases. Such an increase in output
is referred to as an overshoot. Overshoots normally have maximum amplitudes equal
in value to the degree of compression. The overshoot will continue until the input
signal is suitably changed or, if the input signal remains constant at its new high
level, until the control circuit time lag is sufficiently overcome so as to reduce
the gain of the compressor to the gain directed by its compression law. Overshoots
are undesirable because they can overload the channel or device carrying the output
signal from the compressor.
[0015] Various companding systems have approached the problem of overshoots in different
ways: fixed attack times, using a short attack time or a long attack time, and, variable
attack times. A short attack time tends to minimize the amplitude and time of the
overshoot but has an undesirable side effect in that rapid changes in gain cause significant
modulation products to be generated. In order for such modulation products generated
in a compressor to be cancelled, the compressed signal must be carried by a linear
phase channel and the expander must provide reciprocal treatment. Such requirements
are difficult or impossible to meet in practical situations. A long attack time has
the advantage that modulation products are minimized but significant overshoots are
produced. Accordingly, some companding systems have employed arrangements in which
the attack time is variable, remaining relatively long during steady-state signal
conditions but changing to a short attack time during input transients.
[0016] In the A-type system mentioned above, variable attack time control circuits are employed.
In addition, the system is a dual-path arrangement that takes advantage of the fact
that the side paths, in which the limiting takes place, should not have signals exceeding
a predictable maximum amplitude. Accordingly, non-linear clipping is employed in the
side paths as a back-up or secondary overshoot suppression in addition to the variable
shortening of the control signal attack time. Because the signal level in the side
paths are substantially less than that in the main path, the distortion introduced
is small. In addition the non-linear clipping acts very briefly and infrequently.
[0017] As mentioned above, the introduction of the modulation control technique results
in a larger output signal than would occur without modulation control. If modulation
control were incorporated into a dual-path system, such as the A-type system, the
signal in the side path would be larger than otherwise and would not have a predictable
maximum amplitude: the side path signal would continue to rise with the input signal.
Accordingly, a back-up overshoot suppression arrangement in the side path employing
non-linear clipping at a fixed level would not be operable if modulation control were
used.
[0018] The variable attack time control circuits used in the A-type system employ first
and second integrators (smoothing circuits) coupled by components that include "speed
up" diodes that function to decrease the attack time of the control circuit as the
input signal transients become more and more extreme. However, in the absence of a
back-up overshoot arrangement, the minimum attack time of the A-type system variable
attack time control circuits cannot be shortened sufficiently to sufficiently suppress
all overshoots likely to be produced.
[0019] Other known variable attack time control circuits have employed control circuits
having a fixed attack time control path and a rapid attack time control path, both
applied to the device under control. However, a significant drawback to that approach
is that the resulting control signal, resulting from the addition of the signals from
the control paths, has abrupt variations under transient input conditions causing
distortion in the output signal.
Summary of the Invention
[0020] In accordance with the teachings of the present invention, improved control circuits
are provided for use in arrangements for altering the dynamic range of audio signals.
[0021] According to one aspect of the invention, the control circuit of a limiting device
used in a compressor or expander includes a capacitor from which the control signal
is derived, means having a relatively long time constant for charging the capacitor
in response to steady-state input signal conditions, and means for charging the capacitor
very rapidly in response to transient input signal conditions. The invention assures
that the rapid increases in the capacitor voltage charge are accomplished in a controlled
way so that the charge buildup is smooth with minimal discontinuities. In that way,
distortion of the output waveform is minimized.
[0022] The steady-state portion of the control circuit preferably includes two integration
or smoothing stages, but may be implemented using only a single smoothing stage. The
time constant of the single or double smoothing stage is chosen to minimize modulation
distortion without regard to overshoots. The transient portion of the control circuit
includes at least one overshoot suppression circuit for rapidly charging the second
(in the case of two smoothing stages) or the only (in the case of only a single smoothing
stage) smoothing capacitor. In certain arrangements, particularly systems involving
multiple stages, more than one overshoot suppression circuit contributes to rapidly
and smoothly charging the smoothing capacitor. An essential feature, however, is that
the control circuit has at least a primary overshoot suppression circuit which derives
its input from the output signal of the stage which is controlled by the control circuit.
In systems involving multiple stages, additional rapid charging for the capacitor
may be derived from an associated stage in order to achieve a smoother or more accurate
rapid buildup of the capacitor voltage charge than would be achieved using only the
primary overshoot suppression circuit. In stages operating at low frequencies, an
additional charging current, responsive to slow signal buildups, for smoothing discontinuities
in the charging current from the primary overshoot suppression circuit is provided
by a further circuit derived from low frequency components of the output signal of
the stage or an associated stage.
[0023] The rectifiers and smoothing stages of the steady-state portion of the control circuits
must yield a system with accurate characteristics even with phase dispersive transmission
channels. To meet this requirement the rectifier and smoothing stages in the steady-state
portion of the control circuits must at least be average (ideally, but with greater
expense, RMS) responding. It is is not practical, for example, to employ a two stage
smoothing arrangement in which the rectifier and first stage of smoothing has essentially
a zero attack time because the steady-state properties of the control circuit are
disturbed; the circuit would respond to clicks and other anomolies in the signal being
treated.
[0024] It is known to use a small attack time constant (e.g., 1 ms) stage (a peak rectifier,
for example) with a significant holding time (e.g., 10 ms) followed by a further smoothing
stage with a long time constant. To accommodate transients, signals from the first
peak holding circuit are transferred by a speed-up diode or added to the output of
the second smoothing circuit. Such arrangements do not have good accuracy if the information
channel alters the phase relations of the signal components significantly. Furthermore,
the non-zero attack time of the first circuit slows the action of the compressor and
significant overshoots may be produced.
[0025] The basic arrangement of one aspect of the present invention avoids such problems
by employing a long time constant average responding rectifying and smoothing steady-state
path and a separate overshoot suppression path that applies a raw rectified signal
from the output of the variable gain element driving the steady-state path directly
to the final smoothing capacitor. The overshoot suppression path has substantially
a zero attack and decay time constant.
[0026] In a further aspect of the invention, modulation control techniques are employed
and modulation control signals are fed in opposition to both the steady-state and
overshoot suppression circuit portions of control circuits in order that those portions
of the control circuit track each other as a function of signal level and frequency.
Brief Description of the Drawings
[0027]
Figure 1 is a block diagram of a companding system in which the compressor and expander
are configured as Type I devices, each having two side paths, a high frequency stage
and a low frequency stage.
Figure 2 is a block diagram of a companding system in which the compressor and expander
are configured as Type II devices, each having two side paths, a high frequency stage
and a low frequency stage.
Figure 3 is a block diagram of a multi-stage companding system in which the compressor
and expander each have three stages configured as Type I devices.
Figure 4 is a block diagram of the steady-state aspects of a high frequency stage
usable in the arrangements of Figures 1 through 3.
Figure 5 is a block diagram of the steady-state aspects of a low frequency stage usable
in the arrangements of Figures 1 through 3.
Figure 6A is a phasor diagram used in explaining an aspect of the invention.
Figure 6B is a further phasor diagram used in explaining an aspect of the invention.
Figure 7 is a block diagram of the system of Figure 3, showing where modulation control
signals may be derived.
Figure 8 is a block diagram showing the signal processing applied to derive the various
modulation control signals.
Figure 9 is a partially schematic block diagram showing the high frequency stage of
Figure 4 with the addition of transient aspects and the application of modulation
control signals.
Figure 10 is a partially schematic block diagram showing the low frequency stage of
Figure 5 with the application of modulation control signals.
Figure 11 is a partially schematic block diagram showing the low frequency stage of
Figure 10 with the addition of transient aspects.
Figure 12 is a schematic circuit diagram showing the main (steady-state) portion of
the sliding band control circuits.
Figure 13 is a schematic circuit diagram showing the main (steady-state) portion of
the fixed band control circuits.
Figure 14 is a schematic circuit diagram showing the primary overshoot suppression
circuit used in the sliding band and fixed band control circuits.
Figure 15 is a block diagram showing an alternative way of applying the modulation
control signal(s) to the primary overshoot suppression circuit.
Figure 16 is a schematic circuit diagram showing the secondary overshoot suppression
circuit located in the low frequency fixed band stages.
Figure 17 is a schematic circuit diagram showing the low frequency overshoot suppression
circuit.
Figures 18 through 25 are examples of waveforms that are useful in describing the
operation of the overshoot suppression circuits.
Detailed Description
[0028] Although certain aspects of the present invention are usable in the context of other
circuit arrangements, the invention will be described in connection with a three-stage
compressor (and three-stage expander) system, the stages in turn being constructed
of high frequency and low frequency sub-stages. The initial portion of this detailed
description sets forth the environment for the various aspects of the present invention.
[0029] High frequency and low frequency stages of the type set forth in Figures 9-17 can
be used as building blocks in creating compressors, expanders and noise reduction
companders. For example, high frequency and low frequency stages of the type described
in Figures 9-17 may be employed as side paths in dual path arrangements in the manner
shown in Figures 1, 2 and 3.
[0030] United States Patents Re 28,426; 3,846,719; 3,903,485; 4,490,691; and 4,498,055,
referred to in this application, are each incorporated herein by reference, each in
its entirety.
[0031] In Figure 1, a Type I dual path arrangement (of the type generally described in US-PS
3,846,719) is shown having a compressor 8 in which the input signal is applied to
the high frequency stage 10, to the low frequency stage 12 and to the main path 14.
The outputs of stages 10 and 12 are summed in summing means 16 and then summed with
the main path signal components in summing means 18 to provide the compressor output
for application to a transmission channel. The side path signal components thus boost
the main path signal components causing compressor action. The transmission channel
output is applied to the expander 20, configured in a complementary manner to the
compressor 10, having an input summing means 22 which receives the transmission channel
output and subtracts the sum of the high frequency stage 10 and low frequency stage
12 outputs, which are added in summing means 24. The side path signal components thus
buck the main path 26 signal components causing expander action.
[0032] In Figure 2, a Type II dual path arrangement (of the type generally described in
US-PS 3,903,485) is shown having a compressor 28 which has an input summing means
30 receiving the input signal and the sum of the high frequency stage 10 and low frequency
stage 12 outputs, which are combined in summing means 32. The summing means 32 has
its output applied to the main path 34 which provides the compressor output to the
transmission channel and the input to the stages 10 and 12 of the compressor. The
side path signal components thus boost the main path signal components causing compressor
action. The transmission channel output is applied to the expander 36, configured
in a complementary manner to the compressor 28. The input signal is applied to the
high frequency stage 10, to the low frequency stage 12 and to the main path 38. The
outputs of stages 10 and 12 are summed in summing means 40 and then subtracted from
the main path signal components in summing means 42 to provide the expander output.
The side path signal components thus buck the main path signal components causing
expander action.
[0033] In the various dual path Figures, the main path of each compressor and expander is
linear with respect to dynamic range and the level of the sum of the side path high
frequency and low frequency stages is usually less than the maximum level of the main
path. The transmission channel in the various Figures may include any type of storage
or transmission medium and may also include means for converting or encoding the analog
signal components from the compressor into a different form (digital, for example),
the storage or transmission of the encoded signals, and means for re-converting or
decoding the encoded signals back into analog signal components for processing by
the expander.
[0034] In arrangements such as in Figures 1 and 2 where only one high frequency stage and
one low frequency stage are used in each compressor and expander it is practical to
provide a maximum of about 10 to 12 dB of noise reduction without reaching excessive
maximum compression or expansion ratios. Although the arrangements of Figures 1 and
2 will be adequate in certain applications, it is useful to employ the teachings of
US-PS 4,490,691 to achieve a greater amount of overall noise reduction without placing
an undue burden on any one stage or creating excessive compression or expansion ratios.
[0035] In Figure 3, one possible arrangement is shown in which there are three series Type
I dual path stages in the compressor and three complementary stages in the expander.
The threshold levels of the series bi-linear circuits are staggered. Alternatively,
a Type II configuration could be employed. The embodiment of Figure 3 also employs
the spectral skewing and antisaturation aspects of US-PS 4,490,691, although these
aspects are not essential to a multi-stage arrangement employing high frequency and
low frequency stages of the type shown in Figures 9-17.
[0036] The compressor portion of the system of Figure 3 has three stages: a high level stage
44, which has the highest threshold level; a mid-level stage 46; and a low level stage
48, which has the lowest threshold level. In a practical embodiment thresholds of
about -30 dB, -48 dB, and -62 dB (relative to a reference level which is taken to
be about 20 dB below the maximum level in the system), respectively, are employed.
As discussed in US-PS 4,490,691 this is the preferred order of arrangement of staggered
stages, although the reverse order is possible. The expander portion of the system
of Figure 3 also has three stages arranged complementary to the compressor: the low
level stage 50, the mid-level stage 52, and the high level stage 54. Each high level
and mid-level stage has both a high frequency stage 10 and a low frequency stage 12.
The low level stages have only a high frequency stage 10 and no low frequency stage.
Each high frequency stage 10 and each low frequency stage 12 preferably is of the
type described in connection with Figures 6, 7, and 8. In practical circuits there
may be some minor differences between or among high frequency and low frequency stages
depending on whether it is located in the high level, mid-level or low level stage.
[0037] If each compressor stage (44, 46, 48) and each expander stage (50, 52, 54) has, for
example, 8 dB of compression or expansion, respectively, then the overall compander
system will provide 24 dB of noise reduction in the high frequency band (above 800
Hz, if the high frequency stages have an 800 Hz cutoff frequency) and 16 dB of noise
reduction in the low frequency band (below 800 Hz, if the low frequency stages have
an 800 Hz cutoff frequency). Such an arrangement is useful, for example, in a high
quality audio noise reduction system of the type used in professional applications.
[0038] The input to the compressor portion of the system is applied to low frequency and
high frequency spectral skewing networks shown as block 56. In a practical embodiment
the high frequency network is a low pass filter with an attenuation characteristic
like that of a 12 kHz two-pole Butterworth filter but with a limiting attenuation
of about 35 dB (i.e., a shelf response). The low frequency network is a 40 Hz high
pass filter, connected in series with the high frequency network, also with a two-pole
Butterworth-like characteristic but with about a 25 dB limiting attenuation. Complementary
de-skewing networks are located in block 86 at the output of the expander.
[0039] The main paths of the mid-level stage 46 and the low-level stage 48 in the compressor
portion include a low frequency antisaturation network 58 and a high frequency antisaturation
network 60, respectively. Complementary antisaturation networks 62 and 64 are located
in the main path of stages 50 and 52, respectively, in the expander portion. As discussed
in US-PS 4,490,691, it is possible to locate such networks in the main path of only
one stage in the compressor and in the complementary location in one stage in the
expander portion of a series of cascaded staggered stages. In a practical embodiment,
the high frequency and low frequency antisaturation networks are operative above about
4 kHz and below about 100 Hz, respectively. There is an effective compounding of the
antisaturation networks and the spectral skewing networks. The overall result is a
low frequency antisaturation effect of about 10 dB at 20 Hz and 15 kHz.
[0040] The Type I stages of Figure 3 also include summing means 66, 68, 70, and 72 that
combine the outputs of the high frequency and low frequency circuits in stages 44,
46, 52, and 54, respectively. The stages each include summing means 74, 76, 78, 80,
82, and 84 in the main paths which couple to the main path the side path output, in
the case of stages 48 and 50, or the outputs of the side paths, in the case of the
other stages.
[0041] In operation, the main signal paths are primarily responsible for conveying high
level signals. The noise reduction signals from the side paths are additively combined
with the main signal in the encoding mode and subtractively in the decoding mode,
whereby an overall complementary action is obtained. In Figure 3, a dedicated encoder
and decoder are shown laid out in a symmetrical fashion; other decoder configurations
are possible in switchable circuits. For example, as is well known in the art, a complete
encoder can be placed in the negative feedback loop of a high gain amplifier to form
a decoder.
[0042] In Figure 4, the steady-state elements of a high frequency stage 10 are shown. Additional
explanation of the operation of Figure 4 is given in connection with the description
of Figure 9, below. A single pole high pass filter 102 with a cutoff frequency of
about 800 Hz. In practice, the filters throughout the various Figures are configured
as passive RC filters in the inputs of operational amplifiers that act as buffers.
The filtered input signal is applied to a fixed band element 106 and to a sliding
band element 108.
[0043] A fixed band element achieves limiting by providing the same amount of gain reduction
throughout the frequency band in which it operates in response to a dominant signal
component. Fixed band elements can be configured as variable gain or variable loss
devices as discussed in US-PS 4,498,055. An effective and economical implementation
is to employ the source-drain path of an FET as a variable loss device (variable resistor)
by controlling the voltage applied to its gate.
[0044] A sliding band element employs signal dependent variable filtering to achieve limiting.
Generally, a dominant signal component causes the cutoff or turnover frequency (or
frequencies) of one or more variable filters (e.g., high pass, low pass, shelf, notch,
etc.) to shift so as to compress or expand the dominant signal component. A sliding
band system also may be implemented effectively and economically by employing the
source-drain path of an FET as the variable element (variable resistor) of a variable
filter by controlling the voltage applied to its gate as described in US-PS Re 28,426
and US-PS 4,490,691.
[0045] The fixed band element includes an input resistor 110, a shunt variable resistor
112 (the resistor 110 and variable resistor 112 thus functioning as a variable voltage
divider), and a control circuit 114 that generates a DC control voltage which is applied
to the gate of the variable resistor 112. The variable resistor resistance drops as
the DC control voltage level increases, thus increasing attenuation. Fixed band control
circuit 114 includes in its loop a high pass filter 116, having a corner frequency
of about 400 Hz, a further high pass filter 143, having a corner frequency of about
1.6 kHz, a full-wave rectifier 118, a smoothing circuit 120, employed to smooth the
control signal and to adjust the attack and release time constants of the control
loop, and a DC control signal amplifier 122.
[0046] The sliding band element 108 includes parallel input resistor 124 and capacitor 126
which are shunted by variable resistor 128, the overall arrangement thus providing
a variable filter (a variable high pass shelf characteristic that "slides" upward
as the DC control voltage increases). The sliding band element has a control circuit
130 which includes a buffer amplifier 132, a summing means 134, a single pole high
pass filter 136 having a cutoff frequency of about 10 kHz to provide high frequency
emphasis, a full-wave rectifier 138, a smoothing circuit 140, and a DC control signal
amplifier 142. The summing means 134 also receives as inputs bucking signals (signals
that oppose the input from buffer 132) taken before and after high pass filter 143.
The output of the fixed band element 106 is applied to the sliding band element 108
through buffer 144. The overall output is taken from filter 132.
[0047] In operation, the fixed band and sliding band elements operate in a manner that draws
on the best features of both types of circuits. The operation can be described as
"action substitution". In any particular stage, fixed band dynamic action is used
whenever it provides best performance; sliding band operation is substituted whenever
it has an advantage. In this way the best features of both methods are obtained, without
the attendant disadvantages of each.
[0048] The substitution is effective on a continuous and frequency by frequency basis. For
example, the output from a given high frequency stage will typically be from the fixed
band for frequencies up to the dominant signal component and from the sliding band
above that frequency. Conversely, the output from a low frequency stage will be from
the fixed band for frequencies down to a low frequency dominant component and from
the sliding band below that frequency. Thus, the overall circuit behaves like a two-band
fixed band compressor circuit, with an 800 Hz crossover, in the region between any
low and high frequency dominant signal components that may be present; the circuit
responds like a two-band sliding band compressor below and above the frequencies of
the dominant signal components.
[0049] The coupling of bucking signal components from the fixed band element to the control
circuit of the sliding band element are useful in permitting different thresholds
to be set in the elements while retaining adequate control circuit gain in the sliding
band element at frequency extremes.
[0050] In Figure 5, the steady-state elements of a low frequency stage 12 are shown. The
input signal is applied to a fixed band element 150 and to a sliding band element
152. The fixed band element includes an input resistor 154, a shunt variable resistor
156, and a control circuit 158 that generates a DC control voltage which is applied
to the gate of the variable resistor 156. Control circuit 158 includes in its loop
a buffer amplifier 160, a first single pole low pass filter 162 having a corner frequency
of about 800 Hz, a second low pass filter 164 having a corner frequency of about 1.6
kHz, a further low pass filter 192, having a corner frequency of about 400 Hz, a full-wave
rectifier 166, a smoothing circuit 168, employed to smooth the control signal and
to adjust the attack and release time constants of the control loop, and a DC control
signal amplifier 170.
[0051] the sliding band element 152 includes parallel input resistor 172 and inductor 174
which are shunted by variable resistor 176 (a variable low pass shelf characteristic
that "slides" downward as the DC control voltage increases). In practice, the inductor
174 is simulated by a gyrator circuit which includes operational amplifiers (gyrator
circuits are well known). The sliding band element has a control circuit 178 which
includes a single pole low pass filter 180, having a corner frequency of about 800
Hz, a summing circuit 182, a single pole low pass filter 184 having a corner frequency
of about 80 Hz to provide low frequency emphasis, a full-wave rectifier 186, a smoothing
circuit 188, employed to smooth the control signal and to adjust the attack and release
time constants of the control loop, and a DC control signal amplifier 190. Low pass
filter 180 is preferably located in the position shown in order to assist in suppressing
undesired noise or any transient distortion generated in the low frequency stage.
Alternatively, the filter may be located in the input to the arrangement as is done
in the high frequency circuit of Figure 4. The summing circuit 182 also receives an
input bucking signal taken after low pass filter 192. The output of the fixed band
element 150 is applied to the sliding band element 152 through buffer 194. The overall
output is taken from filter 180 of the sliding band element 152.
[0052] In operation, the low frequency stacked fixed band and sliding band elements operate
generally in the manner described above except that the sliding band element operates
downwardly in frequency. One difference in the low frequency stage, as noted above,
is that the band defining filter is located in the stage output rather than in the
input as in the high frequency stage. The 400 Hz filter is also useful for providing
differential control of the sliding band element only at low frequencies.
[0053] In the arrangements of US-PS 3,846,719; US-PS Re 28,426; and US-PS 4,490,691 and
in commercialized embodiments based thereon (marketed and licensed by Dolby Laboratories
and known as the A-type, B-type, and C-type noise reduction systems) the noise reduction
signal (from the side paths) is highly limited under high-level signal conditions.
This high degree of limiting, beginning at a low-level threshold, is responsible for
the low distortion, low overshoot, and low modulation distortion which characterize
these systems.
[0054] As set forth in US-PS 4,498,055, it is is unnecessary to utilize such a low threshold
and such a strong limiting characteristic under certain conditions. In particular,
whenever the noise reduction signal departs from an in-phase condition with respect
to the main path signal, then the threshold can be raised. Furthermore, after an appropriate
degree of limiting has taken place at a given frequency (in order to create the desired
overall compression law), then it is unnecessary to continue the limiting as the signal
level rises. Rather, the level of the noise reduction signal can be allowed to rise
as the input signal rises, stabilizing at some significant fraction of the main path
signal level.
[0055] For example, in the fixed band portions of arrangements such as shown in Figures
4 and 5 the application of the teachings of US-PS 4,498,055 results in conventional
performance in the pass- band (in-phase) frequency region. However, in the stop-band
region the limiting threshold is allowed to rise and the degree of limiting is reduced.
The possibility of doing this can be appreciated by consideration of the phasor diagrams
of the two conditions: Figure 6A which is the phasor diagram of a dual-path compressor
in the pass-band, and Figure 6B which is the phasor diagram of a dual-path compressor
in the stop-band. In the pass-band (in-phase) condition the noise reduction signal
and the main path signal add directly: therefore a relatively low threshold must be
maintained at all pass-band frequencies. Outside the pass-band the effective amplitude
contribution of the noise reduction signal may be minimal due to the phase difference
between it and the main path signal; because of this it is possible to raise the threshold
significantly and to reduce the limiting strength once the desired amount of attenuation
has been obtained at a given frequency.
[0056] Similar considerations apply in sliding band circuits. In the B-type sliding band
circuit (described in detail in US-PS 4,490,691), a variable filter follows a fixed
filter, which has proved to be an efficient and reproducible arrangement. However,
at frequencies outside the pass-band a pure two-pole filter results in overall amplitude
subtraction because of the large phase angles created. Therefore, the type of filter
which has been employed is only quasi-two-pole (a single pole fixed filter plus a
variable shelf characteristic).
[0057] The same arrangement is used in the practical embodiment of the arrangement of Figure
3, with one octave differences in the variable filter quiescent turnover points and
the fixed filter turnover point (as in the B-type circuit). Above the threshold at
a particular frequency the variable filter slides to the turnover frequency needed
to create the overall (main path plus noise reduction signal) compression law. As
the input level rises, and once an overall gain of unity is obtained, there is no
reason for further sliding of the variable filter. At this point the modulation control
arrangement as taught in US-PS 4,498,055 counteracts further sliding of the variable
filter; this prevents unnecessary modulation of the signal and impairment of the noise
reduction effect achieved during decoding.
[0058] The above effects in both fixed and sliding bands are created by circuits called
modulation control circuits. Suitably filtered or frequency weighted signals from
the main signal path are rectified, and in some cases smoothed, and are fed in opposition
to the control signals generated by the control circuits of the various stages. The
result at higher signal levels is to create a balance or equilibrium between the stage
control signals and the modulation control signals. Under these conditions there is
no further gain reduction or sliding of the relevant variable filters with increasing
input signal levels.
[0059] As mentioned in US-PS 4,498,055, when modulation control techniques are embodied
in multistage devices, the modulation control circuits need not be derived from within
each individual stage. Figure 7 shows a preferred arrangement for deriving modulation
control signals for use in an encoder/decoder system such as shown in Figure 3. As
explained further below, eight modulation control signals, designated MC1 through
MC8, are employed. The main modulation control signals MC1-MC7 are derived from the
main path point between the mid-level stages 46 and 52 and the low level stages 48
and 50. In this way the modulation control signals begin to have a significant influence
at relatively low levels, such as at -30 dB (relative to the reference level) because
of the contributions of the high level and mid-level stages; the phase relationships
between the modulation control signals and the signals in the control circuits of
the several stages are also optimized. In the generation of MC8, which is used for
low-frequency stage overshoot-suppression inhibition under high-frequency transient
signal conditions, the influences of the noise reduction stages are undesirable. MC8
is therefore derived from a point between the high level stages 44 and 54 and the
spectral skewing 56 and de-skewing network 86, respectively.
[0060] Figure 8 shows further details of the modulation control circuits. MC1-3 are used
for the high frequency stages 10; MC5-8 are used for the low frequency stages 12.
[0061] MC1 controls the high frequency sliding band circuits. The signal from the takeoff
point is fed through a single-pole high pass filter 202 having about a 3 kHz corner
frequency, full wave rectified in block 204, and fed in opposition to the control
signals generated by the high frequency stages. MC1 is also smoothed by a two-stage
integrator 208 having about a 1 ms (millisecond) time constant and is employed, as
MC2, to oppose the operation of the high frequency sliding band overshoot suppression
circuits (described below); the overshoot suppression thresholds thereby track the
steady state thresholds. MC2 must be smoothed because the phase relationships of MC1
and the signals in the stages vary throughout the audio band (because of the sliding
band action), being a function of frequency and level.
[0062] MC3 controls the high frequency fixed band circuits. The signal from the takeoff
point is weighted by cascaded single-pole low pass filters 210, 212, having respective
corner frequencies of about 400 Hz and about 800 Hz, full wave rectified in block
214, and fed in opposition to both the steady state and transient control circuits
(the transient control circuit or overshoot suppression circuit, as it may alternatively
be called, is described below) of the high frequency fixed band circuits. There is
no need to provide a smoothed MC signal for the overshoot suppression circuits of
the high frequency fixed band circuits because a fixed phase relationship exists between
the signals of the fixed band circuits and the modulation control signal MC3 throughout
the audio band.
[0063] MC4 controls the sliding band circuits of the low frequency stages. The signal from
the takeoff point is fed through a single-pole low pass filter 216, having about a
200 Hz corner frequency, full wave rectified in block 218, and fed in opposition to
the sliding band control signals generated in the stages. MC4 is smoothed by a two-stage
integrator 222, having about a 2 ms time constant, to form MC5; this signal is used
to control the low frequency sliding band overshoot suppression circuits (described
below).
[0064] MC6 controls the low frequency fixed band circuits. The signal from the takeoff point
is weighted by cascaded single-pole high pass filters 224, 226, having corner frequencies
of about 800 Hz and 1.6 kHz, respectively, full wave rectified in block 228, and used
to oppose the steady-state fixed band control signals. MC6 is also smoothed in a two-stage
integrator 230, having a time constant of about 2 ms, forming MC7, which is used to
control the low frequency fixed-band overshoot suppression circuit (described below).
This smoothing is necessary in low frequency fixed-band stages because, unlike the
situation in the high frequency fixed-band stages, there is no fixed phase relationship
between the stage signals and the overshoot suppression signals. MC7 is also used
in a supplemental way to control the low frequency sliding-band overshoot suppressors.
[0065] MC8 is used to control the overshoot suppression circuits of both the fixed and sliding
band low frequency circuits. MC8 compensates for the fact that no frequency weighting
is used in the generation of the low frequency primary overshoot suppression signals.
High frequency transient signal components are detected and used to oppose the operation
of the LF primary overshoot suppression circuits. The signal from the MC8 takeoff
point is fed through a high pass filter 232, having about a 3 kHz corner frequency,
full wave rectified in block 234, double differentiated with approximately 15 microsecond
time-constants in block 236, and peak-hold rectified with about a 30 ms time-constant
in block 238. The resultant high frequency transient modulation control signal MC8
is then employed to oppose the low frequency overshoot suppression action.
[0066] A side effect of the modulation control scheme is that at high signal levels the
amplitudes of the noise reduction signals from the side paths are relatively high
in comparison with the situation in the A-type, B-type, and C-type systems that do
not employ modulation control. Because of this it is not possible to employ simple
overshoot suppression diodes as in these previous systems (for example, clipping diodes
28 in Figure 4 of US-PS Re 28,426). According to one aspect of the present invention,
overshoot suppression side circuits are used in parallel with a portion of the steady-state
control circuit in order to provide a rapid but controlled decrease in attack time
of the control circuit. Under extreme transient conditions, e.g. from a sub-threshold
signal situation, the overshoot suppression threshold is set at its lowest point,
about 10 dB above the relevant steady state threshold.
[0067] The steady-state thresholds in the various circuits are set by adjusting the control
signal amplifier gain or variable gain element as mentioned in US-PS 4,490,691. The
overshoot suppression threshold are set as described below in connection with Figures
14 and 16. By adjusting the gain and bias in the steady-state and overshoot suppression
paths of the control circuits the circuit designer has substantial flexibility in
choosing the level at which the overshoot suppression begins to act and the gradualness
with which it acts once it begins to act.
[0068] With high level steady-state signals and with complex signals (many frequencies)
the threshold rises. The rising thresholds are achieved by applying basically the
same modulation control signals to the overshoot suppression side circuits as to the
steady state portion of the control circuits; since basically the same modulation
control signals are used to control the steady state characteristics, there is a tracking
action between the transient and steady state behavior. This arrangement results in
both well controlled overshoots and low modulation distortion.
[0069] Both primary and secondary overshoot suppression circuits are employed, the latter
acting as fall-back or long-stop suppressors under extreme complex signal conditions
(e.g. high-level low and mid frequency signals in combination with high-level frequency
signals). In the low frequency circuits a further overshoot suppressor is used for
very low frequency signals; this is a very gentle, slow acting circuit which reduces
low frequency transient distortion.
[0070] Figure 9 adds the modulation control features and overshoot suppression circuit features
to the steady-state high frequency stage described in connection with Figure 4. Thus,
Figure 9 shows both the steady-state and transient control aspects of the high frequency
stages. As with other block diagrams, this figure shows only the basic parameter determining
elements; the practical circuits of course contain other details such as buffering,
amplification, and attenuation. The high-level, mid-level, and low-level stages (of
Figure 3) have the same basic block diagrams and schematics. The main distinctions
are that the AC and DC circuit gains are increased for the mid- and low-level stages.
[0071] Referring to Figure 9, as in Figure 4, each stage comprises a fixed band section
on the bottom and a sliding band section on the top, each with its own control circuits.
The same reference numerals are used for like elements in Figures 4 and 9. The fixed
and sliding band circuits are fed in parallel and the output signal is taken from
the sliding band circuit. The sliding band variable filter is referenced to the output
of the fixed band; that is, the fixed band output is fed directly to the bottom end
of the sliding band variable resistor 128. This connection results in the action substitution
operation mentioned previously. The overall output will always be the larger of the
fixed and sliding band contributions at all frequencies. If there is a signal situation
in which the fixed band output is negligible, then the sliding band takes over. Conversely,
if there is little or no sliding band contribution, the output from the fixed band
will still feed through to the output through the sliding band variable resistor 128.
In this way the action of one circuit is substituted for that of the other circuit
as the occasion requires.
[0072] The incoming signal is fed through a single-pole high pass filter 102, having a corner
frequency of about 800 Hz. The output signal is taken from the sliding band stage
and is fed through buffer 132. Thus, the overall quiescent (sub-threshold) frequency
response of the circuit is that of a single-pole 800 Hz high pass network. The low
frequency stages have a complementary 800 Hz single-pole low pass characteristic,
which overall results in optimal combination of the signals from the high and low
frequency stages.
[0073] The fixed band output from the fixed band variable resistor 112 is fed via weighting
filter 116 to two control circuits, the main (pass-band and stop-band) control signal
circuit 252 and the pass-band control circuit 254. This arrangement is similar to
Figure 21 of US-PS 4,498,055. In the main control circuit the signal is full wave
rectified (all control circuit rectifiers in the system are full wave) in block 256
and opposed in combining means 258 by the modulation control signal MC3. The resulting
DC signal is smoothed by a smoothing circuit 260 with about an 8 ms time constant
(the overall steady-state control signal characteristic in this and all other stages
is average responding--an important feature in a practical companding system). The
control signal is then fed to one input of a maximum selector circuit 262, which passes
to its output the larger of two signals applied to the input.
[0074] The fixed band output is also fed to the pass-band control circuit 254, which comprises
the 1.6 kHz single-pole high pass filter 143, a rectifier 266, and a smoothing circuit
(about 8 ms) 268. The pass-band control signal is applied to the other input of the
maximum selector circuit. The output of the maximum selector circuit is further smoothed
by about a 160 ms time constant in block 270 and is used to control the fixed band
variable resistor 112 via variable resistor driver 122.
[0075] The dual control circuit arrangement described above is employed to obtain optimal
performance under both simple signal (single dominant signal) and complex signal (more
than one dominant signal) situations. The modulation control signal MC3 is optimized
in frequency weighting and amount for simple signal conditions, in which the modulation
control action is most useful. Under complex signal conditions, however, the modulation
control signal developed becomes larger, and the subsequent modulation control action
is then greater than necessary; that is, the DC control signal output from the main
control circuit is less than required. Under this condition the control signal from
the pass-band circuit is phased in, via the maximum selector circuit, to control the
overall action of the fixed band compressor circuit.
[0076] The output of the fixed band element is fed through buffer 144 with an overall gain
of unity to provide the reference for the sliding band filter; this is the only signal
output of the fixed band circuit.
[0077] The sliding band control signal is derived from the stage output. The signal is fed
through the 10 kHz single-pole high pass weighting network 136 and is rectified. The
rectified signal is opposed in combining means 272 by modulation control signal MC1;
since MC1 also has a single-pole high pass characteristic, the ratio between the rectified
control signal and MC1 monitors the signal attenuation (this ratio creates an end-stop
effect on the sliding band action). The result is smoothed first in block 274 by a
time constant of about 8 ms and finally in block 276 by a time constant of about 75
ms. The smoothed control signal is then used to control the sliding band variable
resistor 128 via variable resistor driver 142. A single control circuit suffices in
the sliding band circuit because the 10 kHz high pass control weighting network 136
tends to offset the effect of complex signals on the modulation control voltage developed
(MC1).
[0078] A modification is made in the control characteristic at low levels. Signals from
the fixed band circuit are combined in combining means 134 in opposition with the
sliding band output signal. The effect is in the direction of simulating the derivation
of the sliding band control voltage from the voltage across the sliding band variable
filter only (i.e. from the voltage across variable resistor 128). This tends to raise
the sliding band threshold at high frequencies, which reduces unnecessary sliding
of the band. The 10 kHz control weighting network provides the correct amount of control
signal for the variable filter at medium and high levels, but it produces the undesirable
side effect of lowering the threshold at high frequencies; the differential control
signal derivation method counteracts this threshold lowering effect.
[0079] The overshoot suppression arrangements for the high frequency stages are also shown
in Figure 9. In the high frequency circuits a general feature is that unsmoothed rectified
signals from the control circuit rectifiers 256 and 138 are opposed by appropriate
modulation control signals and are fed via diode means to the final smoothing circuits
270 and 276, respectively, particularly the capacitors therof. The low frequency arrangements
follow the same pattern, with some modifications as described below.
[0080] In common with the A-type, B-type, and C-type systems, the overshoot suppression
thresholds in the present arrangements are significantly higher than the steady-state
thresholds. Preferably, the low level overshoot suppression levels are set at about
10 dB above the relevant steady-state thresholds; the overshoot suppression effects
are then phased in gradually. The net result is that for most musical signals the
overshoot suppressors rarely operate; the compressors are controlled by well smoothed
signals. When the suppressors do operate, the effect is so controlled that modulation
distortion is minimal. Under relatively steady-state, but nonetheless changing, signal
conditions the overshoot suppression effects are gradually phased out with increasing
signal levels; this action further ensures low overall modulation distortion from
the system. The circuit configuration gives the circuit designer the ability to adjust
the relative thresholds and the gradual phase in of the overshoot effects. As mentioned
above, the thresholds are set by adjusting the gain and bias of the amplifiers in
the steady-state and overshoot suppression circuits. As explained in further detail
below, the gradual phasing in of overshoot suppression effects is accomplished by
operating the coupling diodes (coupling the overshoot suppression circuits to the
capacitor from which the control signal is derived) as variable resistors. Other,
more complex circuits may be employed to achieve this function. Also explained in
greater detail below, the gradual phasing out of overshoot effects is achieved by
limiting circuits that reduce the gain of the overshoot suppression circuits at very
high levels as well as by the modulation control signals that oppose the overshoot
suppression signals at high levels.
[0081] Referring again to Figure 9, in the high frequency fixed band circuit the overshoot
suppression signal is derived from rectifier 256 of the main control circuit 252.
As with the steady-state control signal, the rectified signal is opposed by MC3 in
combining means 278, so that the overshoot suppression threshold is appropriate for
conditions in the steady-state regime. The apropriate AC and DC conditions are set
in amplifier stage 279. As compared with the steady-state circuit, the gain of the
overshoot suppression side circuit is less than unity. The resultant overshoot suppression
signal is coupled by a diode means 280 to the final smoothing circuit 270, particularly
the capacitor thereof.
[0082] In the sliding band circuit two overshoot suppression signals are used, primary and
secondary. The primary overshoot suppression signal is derived from the control circuit
rectifier 138, opposed in combining means 282 by MC2, a smoothed version of MC1 (MC1
controls the steady-state characteristics), the appropriate AC and DC conditions are
set in amplifier stage 283, and coupled to the final smoothing circuit 276, particularly
the capacitor thereof, via diode means 284. As in the fixed band, the gain of the
overshoot suppression side circuit is less than unity. The smoothing of MC1 to create
MC2 is necessary because, unlike the situation in the fixed band circuit, there is
no constant and favorable phase relationship between the signal in the control circuit
and MC1 (because of the sliding band); the smoothing enables reliable and effective
bucking action to take place.
[0083] The effect of the primary overshoot suppression circuit preferably is maximized for
the most significant transient signal situation--that is, a single impulse or tone
burst starting from a sub-threshold signal level. However, under certain signal conditions,
especially those in which relatively steady-state high frequency signals at high levels
are present, a side effect of the use of a smoothed MC2 signal is that the overshoot
suppression level for low and medium frequency transient signals is raised. To overcome
this effect a secondary overshoot suppression signal is derived from the fixed band
overshoot suppression signal and is coupled via diode means 286 to the sliding band
final smoothing circuit 276, particularly the capacitor thereof; the secondary overshoot
suppressor has a higher threshold than the primary suppressor and operates only rarely
because of the unusual circumstances for which it was designed.
[0084] It may be noted that of all the compressor and expander circuits in the system, the
high frequency fixed bands uniquely require only a single overshoot suppressor, which
combines both the primary and secondary functions. In these circuits the phase relationships
of the modulation control signal MC3 and the signals used to derive the control signals
are essentially ideally matched, whereby it is unnecessary to employ any modulation
control smoothing to obtain optimal bucking action.
[0085] Figure 10 shows the steady-state layout of the low frequency stages as in Figure
5 along with the modulation control aspects of the arrangement. As with the high frequency
stages, only the basic parameter determining elements are shown. The high level and
mid-level low frequency stages have the same block diagrams and circuits, but the
AC and DC gains are increased for the mid-level stage.
[0086] Referring to the Figure 10, certain similarities and differences may be noted with
respect to the high frequency stage described in connection with Figure 9. The dual-layer
arrangement of the fixed band on the bottom and the sliding band on the top is similar.
However, the sliding band acts downwardly, using a simulated inductance (gyrator circuit).
As with the high frequency stages, the fixed and sliding band circuits are fed in
parallel, and the output signal is taken from the sliding band circuit. The fixed
band output is coupled to the bottom of the sliding band to provide the action substitution
operation discussed previously.
[0087] A notable difference from the high frequency circuit is that the fixed 800 Hz band
determining filter follows, rather than precedes, the variable filter. This arrangement
has several advantages: a) overshoot suppression signals can be generated without
the delay inherent in a low pass filter, resulting in lower transient distortion,
b) any transient distortion produced by the circuit is attenuated by the 800 Hz low
pass filter, and c) noise generated by the gyrator is attenuated by the filter.
[0088] Referring to the fixed band section 150, the incoming signal is applied directly
to the variable attenuator circuit provided by resistor 154 and variable resistor
156. Control circuit frequency weighting is provided by cascaded single-pole 800 Hz
and 1.6 kHz low pass filters 162, 164. The main control circuit 302 rectifies the
filtered signal in block 304; the resulting DC signal is bucked by modulation control
signal MC6 in combining means 306, smoothed in block 308 by a smoothing circuit with
about a 15 ms time constant, and fed to one input of the maximum selector circuit
310. The maximum selector circuit has the same purpose and mode of operation as in
the high frequency circuits.
[0089] The 800 Hz and 1.6 kHz frequency weighted output of the fixed band circuit is also
fed to the pass-band control circuit 312. Here the control signal is further weighted
by a 400 Hz single-pole low pass filter 192, rectified in block 316, smoothed by a
smoothing circuit with about a 15 ms time constant in block 318, and fed to the other
input of the maximum selector. The larger of the two signals is passed to the final
smoothing circuit (about 300 ms) 320 to become the fixed band control signal applied
to variable resistor 156.
[0090] As in the high frequency circuits, the sliding band control signal is derived from
the stage output--that is, from a point following both the fixed 800 Hz band determining
filter and the variable filter. The signal is frequency weighted by an 80 Hz single-pole
low pass filter 184, rectified in block 186, and bucked in combining means 322 by
modulation control signal MC4 (which also has a single-pole low pass characteristic,
with the same type of sliding band end-stop effect as in the high frequency circuits).
The result is smoothed by a smoothing circuit 324 with about a 7.5 ms time constant
and finally smoothed by a smoothing circuit 326 with a time constant of about 150
ms to become the sliding band control signal applied to variable resistor 176. As
in the high frequency stages, a single control circuit suffices for the sliding band.
[0091] The same type of low level control characteristic modification is made in the low
frequency circuits as in the high frequency circuits. Namely, a signal from the fixed
band is combined in opposition with the sliding band output signal in combining means
182. The modification raises the sliding band threshold at low frequencies.
[0092] Figure 11 adds the overshoot suppression circuitry to the low frequency stage shown
in Figure 10. In a manner generally similar to that of the high frequency circuits,
unsmoothed rectified signals derived from the outputs of the variable elements are
opposed by appropriate modulation control signals and are fed via diode means to the
final smoothing circuits, especially the capacitor in each such circuit.
[0093] Both the fixed and sliding bands each have primary and secondary overshoot suppression
circuits, which operate at frequencies above about 100 Hz. Additionally, both have
gentle and slow-acting low frequency overshoot suppression circuits, operating at
frequencies below about 200 Hz; there is a crossover effect between the two types
of overshoot suppression in the 100-200 Hz region. As in the high frequency circuits,
the primary overshoot suppression circuits provide the earliest and strongest suppression
effect in simple transient situations. With more complex signals the primary overshoot
suppression thresholds rise as the modulation control signal(s) oppose the overshoot
suppression action and eventually the secondary overshoot suppression circuitry takes
control.
[0094] In contrast with the high frequency situation, the low frequency general strategy
is to derive the primary control signals from signal points that do not include any
circuit control frequency weighting. This is because the required control circuit
weighting networks of the low frequency stages are low-pass in character, resulting
in delays (the high-pass networks used for control circuit weighting in the high frequency
stages do not introduce delays). However, because of the lack of a weighting factor
in the primary control signal, there is no inherent tracking between the steady-state
and overshoot suppression thresholds of the circuits involved, particularly in the
stop-bands. Therefore, further modulation control techniques are employed to obtain
the required tracking. The secondary overshoot suppression signals are derived from
a point in the fixed band circuitry that provides adequate tracking in both the fixed
and sliding bands.
[0095] Referring to Figure 11, the fixed band primary overshoot suppression signal is generated
by passing the variable attenuator output through a 200 Hz single-pole high pass filter
352. This filter reduces the influence of the primary overshoot suppression circuit
at low frequencies, allowing the more gentle low frequency overshoot suppression circuit
to take over the transient control function. The signal is full wave rectified in
block 354 and then opposed in combining means 356 by modulation control signal MC7,
a 2 ms (approximately) smoothed version of MC6, the fixed band steady-state modulation
control signal; the effect is in the direction of improving the steady-state and overshoot
suppression threshold tracking on a steady-state basis. However, the thresholds must
also track on a transient basis. This is the function of the high frequency transient
modulation control signal MC8, which is a high-frequency weighted, peak-detected
signal that opposes the primary overshoot suppression signal in the time interval
before MC7 becomes effective. The appropriate AC and DC conditions are set in amplifier
357 and the overshoot suppression signal is then coupled via diode means 358 to the
final smoothing circuit 320, especially the capacitor thereof, of the fixed band circuit.
The gain of the overshoot suppression side circuit is less than the gain of the steady-state
control circuit.
[0096] In the generation of the sliding band primary overshoot suppression signal the output
of the variable filter is fed through a 200 Hz single-pole filter 360 to reduce the
effect of the circuit at low frequencies, as in the fixed band circuit. The signal
is full wave rectified in block 362 and then opposed in combining means 364 by modulation
control signals MC5 and MC7 to provide an adequate degree of tracking between the
steady-state threshold and the overshoot suppression threshold on a steady-state
basis. As in the fixed band circuit, MC8 provides the required degree of tracking
on a transient basis. The appropriate AC and DC conditions are set in amplifier 365
and the resultant overshoot suppression signal is coupled via diode means 366 to the
sliding band final smoothing circuit 326, especially the capacitor thereof. The gain
of the overshoot suppression side circuit is less than the gain of the steady-state
control circuit.
[0097] The secondary overshoot suppression signals for both the fixed band and sliding band
are generated from the frequency weighted point 368 (at the output of the 800 Hz low
pass filter 162 and the 1.6 kHz low pass filter 164) in the fixed band steady-state
control circuit. To prevent interference with the low frequency overshoot suppression
circuit at low frequencies, the signal is further filtered by a 200 Hz single-pole
high pass network 370, as in the primary overshoot suppression circuits; the filtered
signal is then rectified in block 304. On a steady-state basis the pass-band control
circuit 312 controls the circuit at very low frequencies, via the maximum selector
circuit; this arrangement allows the main control circuit rectifier 304 to serve a
double function. The DC signal is opposed by MC6 in combining means 372, so that an
optimal phase relationship is obtained between the rectified signal and MC6, apart
from the effect of the 200 Hz filter 370 (which is negligible). An ideal tracking
effect is also achieved between the steady-state and secondary overshoot suppression
thresholds.
[0098] The effect of the 800 Hz and 1.6 kHz frequency weighting networks 162, 164 is to
introduce a time delay into the secondary overshoot suppression signal. The effective
delay is significantly reduced by using a higher (approximately times two) gain in
the secondary overshoot suppressor circuit than in the primary circuit and applying
limiting in block 374 (thus the effective rise time of the waveform is shortened).
The resultant overshoot suppression signal is more in the nature of a nearly fixed
amplitude impulse, applied in the rare circumstances when necessary, than it is a
proportional response. The signal is coupled through diode 376 means to the fixed
band final smoothing circuit 320, especially the capacitor thereof, and is also used,
suitably biased (see Fig. 16, below, the feed is via resistors 600 and 602, the former
having a value of about 2 kilohms while the latter has a value of about 47 kilohms),
for secondary overshoot suppression in the sliding band circuit, also coupled through
diode means 378.
[0099] The low frequency overshoot suppression signal is developed by tapping at point 380
the rectified, but unsmoothed, output of the pass-band control circuit 312 of the
fixed band circuit. The signal is opposed in combining means 382 by MC6 to desensitize
the circuit to high-level, high frequency components. The signal is further opposed
by the resulting fixed band smoothed control signal from the final smoothing circuit
320, in a negative feedback fashion (when the fixed band control signal has risen
to a sufficient level, there is no further need for any LF overshoot suppressor action.)
The signal is then highly amplified and limited in block 384, peak rectified in block
386, and smoothed by a smoothing circuit 388 having about a 20 ms decay time constant.
The resulting high amplitude pulses are fed through a differentiating network 390,
with a time constant of the same order as the smoothing time constant, to provide
low frequency overshoot suppression impulses of defined strength for distribution
to the fixed band and sliding band final integrators, via high value resistors 392,
394 and series diode means 396, 389, respectively. The result is a decaying "constant
current" charging of the capacitors of the final smoothing circuits. This is in contrast
with the higher peak currents and correspondingly more abrupt control voltage changes
produced by the relatively low-impedance primary and secondary overshoot suppressors.
The use of the low frequency overshoot suppression method results in low waveform
distortion of relatively slowly changing low-frequency signal impulses applied to
the system. Additional explanation of the low frequency overshoot circuit is given
below in connection with the description of Figure 17.
[0100] Figure 12 is a schematic diagram showing the circuit details of the main (steady
state) portion of the sliding band control circuits employed in the high frequency
and low frequency stages. The circuit is fed from filter 136 in the high frequency
stage (Figure 9) and from filter 184 in the low frequency stage (Figure 11). The full
wave rectifier (138, Fig. 9; 186 Fig. 11) employs the technique in which double the
output of a unity gain inverting half wave rectifier is added to the input signal.
Thus, the input signal is applied through resistor 402 to the inverting input of operational
amplifier 404, the non-inverting input of which is connected to minus 9 volts. Diodes
406, 408, resistor 410, input resistor 402, and operational amplifier 404 operate
as a half-wave rectifier. The input signal is fed to a summing point 415 (282, Figure
9; 322 Figure 11) through summing resistor 414 which has double the resistance of
summing resistor 412 that receives the half-wave rectifier output. The same full wave
rectification technique is used throughout the various circuits: however, other full
wave circuits may be used. In the high frequency stages, the input signal and the
half-wave rectifier output are applied to summing resistors in the overshoot suppression
side circuit (Figure 14, below). The summing node 415 also has applied to it the bucking
modulation control input via a summing resistor 416. The modulation control input
"bucks" the other signals at node 415 in the sense that it tends to reduce their amplitude.
In the high frequency stage the modulation control input is MC1; in the low frequency
stage it is MC4. The modulation control arrangement is similar to that described in
US-PS 4,498,055, particularly Figure 11 thereof.
[0101] The summing node operates in cooperation with operational amplifier 418 that functions
not only as a summing amplifier but also as the first smoothing circuit (274, Fig.
9; 324, Fig. 11). The input is applied to the inverting input of amplifier 418 and
its non-inverting input is connected to minus 9 volts. Capacitor 420, resistor 422,
and diode 424 are connected in parallel in the feedback path of amplifier 418. The
first smoothing stage time constant is about 8 ms. In certain relatively non-critical
applications it is possible to eliminate the first smoothing stage entirely.
[0102] The first smoothing circuit output is applied to the second smoothing circuit stage
(276, Fig. 9; 326, Fig. 11). The second smoothing stage includes the main smoothing
resistor 428 and the smoothing capacitor 444 having a time constant of about 75 ms
in the high frequency stages and about 150 ms in the low frequency stages. The charging
path includes a lower valued resistor 426 to provide a suitable point, the junction
of resistors 426 and 428, for the connection a limiter diode 430. Resistor 432 connected
to the nominal positive supply voltage of plus 9 volts and resistor 434 connected
to the reference potential bias the diode. The bias is set so that under extremely
high level high frequency conditions the signal going to the controlled variable resistive
element (implemented using a FET) does not go up into the gate conduction region of
the FET (conduction of the FET may cause an audible thump in the output of the system).
A low valued resistor 442 is located in series with the second smoothing circuit capacitor.
[0103] The second smoothing circuit capacitor 444 also receives charging inputs from several
overshoot suppression circuits. In the high frequency stages the inputs are from the
primary overshoot suppression circuit (Figure 14) forming part of that high frequency
sliding band circuit through diode 184 (Fig. 9) and a secondary overshoot suppression
input via diode 186 (Fig.9) from the primary overshoot suppression circuit associated
with the related high frequency fixed band circuit. Resistor 442 buffers the output
of the overshoot suppression circuits to prevent the operational amplifier in those
circuits from going into high frequency oscillation. All of the charging inputs, the
steady-state input from the first smoothing circuit and the inputs from the overshoot
suppression circuits contribute to the charging of the second smoothing circuit capacitor,
from which the control signal is derived.
[0104] A DC control amplifier (FET driver) 446 (142, Fig. 9; 190, Fig. 11) drives the sliding
band FET (variable resistor 128, Fig. 9) in accordance with the voltage on the second
smoothing circuit capacitor 444.
[0105] Figure 13 is a schematic diagram showing the circuit details of the main (steady
state) portion of the fixed band control circuits employed in the high frequency and
low frequency stages. The arrangement of pass-band and main (pass-band plus stop-band)
sub-circuits and the application of the modulation control signal to the main sub-circuit
is similar to that described in US-PS 4,498,055, particularly Figure 21 thereof.
[0106] The input signal to the main portion (252, Fig. 9) of the control circuit is derived
directly from the fixed band element 106 (Fig. 9) output via a buffer amplifier (not
shown) in the high frequency stages. In the low frequency stages, the main portion
(302, Fig. 11) of the control circuit is derived from the output of filter 164 (Fig.
11) through the 200 Hz high pass filter 370 (Fig. 11). The stop-band portion of the
control circuit has a full wave rectifier (256, Fig. 9; 304, Fig. 11) configured in
the same way as the full wave rectifier in the circuit of Figure 12. The full wave
rectifier includes operational amplifier 454, input resistor 452, diodes 456, 458,
feedback resistor 460, and summing resistors 462 and 464. In the high frequency stages,
the input signal and the half-wave rectifier output are applied to summing resistors
in the overshooot suppression side circuit (Figure 14, below). The summing node 465
(258, Fig. 9; 308, Fig. 11) receives the full wave rectifier output and also has applied
to it the bucking modulation control input via a summing resistor 466. The modulation
control input bucks the other signals at node 258 in the sense that it tends to reduce
their amplitude. In the high frequency stage the modulation control input is MC3;
in the low frequency stage it is MC6.
[0107] The summing node operates in cooperation with operational amplifier 468 that functions
not only as a summing amplifier but also as the first smoothing circuit (260, Fig.
9; 308, Fig. 11). The input is applied to the inverting input of amplifier 468 and
its non-inverting input is connected to minus 9 volts. Capacitor 470 and resistor
472 are connected in parallel in the feedback path of amplifier 468. Diodes 474 and
476 are connected so as to form a maximum selector circuit (262, Fig. 9; 310, Fig.
11). In the high frequency stages the first smoothing circuit time constant is about
8 ms; in the low frequency stages, about 15 ms.
[0108] The pass-band portion (254, Fig. 9) of the control circuit is derived directly from
the fixed band element 106 (Fig. 9) output via a buffer amplifier (not shown) and
via 1.6 kHz high pass filter 143 in the high frequency stages. In the low frequency
stages, the pass-band portion (312, Fig. 11) of the control circuit is derived from
the output of filter 164 (Fig. 11) through the 400 Hz low pass filter 192 (Fig. 11).
The pass-band portion of the control circuit also has a full wave rectifier (266,
Fig. 9; 316, Fig. 11) configured in the same way as the full wave rectifier in the
circuit of Figure 12. The full wave rectifier includes operational amplifier 484,
input resistor 482, diodes 486, 488, feedback resistor 490, and summing resistors
492 and 494. The summing resistors operate in cooperation with operational amplifer
496 that functions not only as a summing amplifier but also as the first smoothing
circuit (268, Fig. 9; 318, Fig. 11). The input is applied to the inverting input of
amplifier 496 and its non-inverting input is connected to minus 9 volts. Capacitor
498 and resistor 472 are connected in parallel in the feedback path of amplifier 468.
In the high frequency stages the first smoothing circuit time constant is about 8
ms; in the low frequency stages, about 15 ms. Resistor 502 couples the output of the
pass-band first smoothing circuit stage to the maximum selector.
[0109] The maximum selector output is applied to the second smoothing circuit stage (270,
Fig. 9; 320, Fig. 11). The second smoothing circuit includes the main smoothing resistor
504 and the smoothing capacitor 514 having a time constant of about 160 ms in the
high frequency stages and about 300 ms in the low frequency stages. A low valued resistor
512 is located in series with the second smoothing circuit capacitor.
[0110] The second smoothing circuit capacitor 514 also receives at least one other charging
input: one input (in the high frequency stages) and three inputs (in the low frequency
stages). In the high frequency stages the input is from the primary overshoot suppression
circuit (Figure 14) forming part of that high frequency fixed band circuit through
diode 280 (Fig. 9). In the low frequency stages, the inputs are from the primary overshoot
suppresion circuit (Figure 14) forming part of that high frequency fixed band circuit
through diode 385 (Fig. 11), the secondary overshoot circuit (Figure 16) also forming
part of that high frequency fixed band circuit through diode 376 (Fig. 11), and the
low frequency overshoot circuit (Figure 17) also forming part of that high frequency
fixed band circuit through diode 396 (Fig. 11). Resistor 512 buffers the output of
the overshoot suppression circuits to prevent the operational amplifier in those circuits
from going into high frequency oscillation. All of the charging inputs, the steady-state
input from the first smoothing circuit and the one or more inputs from the overshoot
suppression circuits contribute to the charging of the second smoothing circuit capacitor,
from which the control signal is derived.
[0111] A DC control amplifier (FET driver) 516 (122, Fig. 9; 170, Fig. 11) drives the fixed
band FET (variable resistor 112, Fig. 9; variable resistor 156, Fig. 11) in accordance
with the voltage on the second smoothing circuit capacitor 514.
[0112] Figure 14 shows the primary overshoot suppression side circuit used in both the sliding
band and fixed band portions of the high frequency and low frequency stages. Some
aspects of the circuit are described above in connection with the descriptions of
Figures 9 and 11. A summing node 549 (282 in sliding band portion of the high frequency
stage of Fig. 9; 278 in the fixed band portion; 364 in the sliding band portion of
the low frequency stage of Fig. 11; 356 in the fixed band portion) at the inverting
input of operational amplifier 550 has a plurality of summing resistors connected
to it. Summing resistors 546 and 548 are from a full-wave rectifier (in the high frequency
sliding band circuit, from full-wave rectifier 138 in the main control circuit [Fig.
9]; in the high frequency fixed band circuit, from full-wave rectifier 256 in the
main control circuit [Fig. 9]; in the low frequency sliding band circuit, from full-wave
rectifier 362 in the overshoot suppression circuit side path [Fig. 11]; in the low
frequency fixed band circuit, from full-wave rectifier 354 in the overshoot suppression
circuit side path [Fig. 11]). Summing resistor 552 is representative of one or more
separate summing resistors from one or more modulation control signal inputs. In the
high frequency sliding band circuit, the input is MC2; in the high frequency fixed
band circuit the input is MC3. In the low frequency sliding band circuit the inputs
are MC5, MC7, and MC8; in the low frequency fixed band circuit the inputs are MC7
and MC8.
[0113] Operational amplifier 550 functions as a summing amplifier and also to set the appropriate
AC and DC conditions for its overshoot suppression output signal which is coupled
to the second smoothing stage of the various sliding band and fixed band circuits
via coupling diode 568 (284 in the sliding band circuit of the high frequency stage,
Fig. 9; 280 in the fixed band circuit, Fig. 9; 366 in the sliding band circuit of
the low frequency stage (Fig. 11); 346 in the fixed band circuit). As explained further
below, coupling diode 568 is used as a variable resistor to provide a voltage dependent
charging current by adjusting the operating parameters so that it operates in the
knee of its forward-biased operating characteristic. The gain of the side circuit
of Figure 14 is slightly less than the gain of the steady-state circuit with which
it is associated. This difference in relative gains is essential to the overall operation,
as explained further below. Diode 554 provides temperature compensation for diode
568. Resistor 560 biases diode 554 into conduction. Resistor 558 is the feedback resistor
for the operational amplifier. Resistor 562 is adjusted to bias the amplifier so as
to provide the optimum DC voltage relative to that of the steady-state circuit. Diode
556 prevents the output from swinging to the negative supply rail: under certain input
conditions, if the modulation control signal applied to the overshoot suppression
circuit is opposing the signal from the full-wave rectifier very much, the signal
in the amplifier 550 could otherwise be forced out of its linear operating region
down to the negative supply rail, thus slowing down the amplifier. Diode 566 and resistor
564 function to decrease the aggressiveness of the overshoot suppression action at
high input levels: the size of the overshoot suppression signal is limited at high
input signal levels.
[0114] Figure 15 shows in block diagram form an alternative form of the circuit of Figure
14. In this alternative, the operational amplifier 550 of Figure 14 is operated as
a variable gain amplifier, controlled by the modulation control signal input such
that as the modulation control signal increases, the gain of the amplifier decreases.
The limiter 572 can be provided by an arrangement such as diode 566 and resistor 564
in the circuit of Figure 14. Optionally, the modulation control signal may also be
applied in a smaller proportion than in the circuit of Fig. 14 so as to buck (oppose)
the input or output of the variable gain amplifier before or after limiter 572, in
summing circuit 574. A further operational amplifier can be employed as a summing
amplifier. The output of the summing circuit is then applied to a coupling diode 576.
Although the alternative arrangement of Figure 15 requires additional circuit components,
it would allow more exact control of the overshoot suppression circuit and better
tracking with the steady-state portion of the control circuit.
[0115] Figure 16 shows the secondary overshoot suppression side circuit in the fixed band
circuit of the low frequency stage. Some aspects of the circuit are explained above
in connection with the description of Figure 11. Its output is used in both the fixed
band and sliding band portions of the low frequency stage. A summing node 372 at the
inverting input of operational amplifier 588 has three summing resistors connected
to it. Summing resistors 580 and 582 are from full-wave rectifier 304 in the low frequency
fixed band circuit (Fig. 11). Operational amplifier 588 functions as a summing amplifier
and also as a limiter. Resistor 590 is a feedback resistor. Diode 594 and resistor
592 provide the same function as diode 566 and resistor 564 in the circuit of Figure
14. In addition, diode 594 functions to provide temperature compensation for the coupling
diodes (598 and 604). Resistor 596 biases the diode 594 into conduction during signal
transients, providing limiting. During this time the diode is also providing temperature
compensation. The output to the capacitor of the low frequency fixed band second smoothing
circuit is taken through diode 598. The output to the low frequency sliding band capacitor
is taken through diode 604 via a biasing network made up of resistors 600 and 602.
[0116] Figure 17 shows the details of the low frequency overshoot side circuit, some aspects
of which are described above in connection with the description of Figure 11. The
inputs at summation point 382 at the input of operational amplifier 620 are taken:
from the full-wave rectifier 316 (Fig. 11) in the pass-band portion of the low frequency
fixed band control circuit via feed resistors 610 and 612; from MC6 (applied so as
to buck the other signals) via resistor 614; and from the second smoothing circuit
320 (Fig. 11) in the low frequency fixed band control circuit. The latter input is
via an operational amplifier 615 and summing resistor 616. The feed from the second
smoothing circuit is applied to the non-inverting input, the output is fed back directly
to the inverting input and the feed is taken from that point--this negative feedback
arrangement causes the feed to buck the input signals from the full-wave rectifier
316 (Fig. 11), thus phasing out the low frequency overshoot action when the fixed
band control signal has risen to a sufficient level. There is no need to continue
the slow charging effect provided by the low frequency overshoot circuit after the
voltage on the smoothing chapacitor has risen far enough.
[0117] The low frequency overshoot suppressor circuit operates only at low frequencies because
MC6, which has a high pass characteristic, is fed in, in opposition to the signal
from the full-wave rectifier. The bucking MC6 signal nullifies effects at high frequencies
by cancelling out high frequency components in the signal received from the full-wave
rectifier. Resistor 618 connected between point 382 and the negative nine volt supply
biases the operational amplifier 620.
[0118] The operational amplifier 620 has a relatively high value of feedback resistor 622
causing the amplifier gain to be sufficient so that its output reaches the supply
rail, thus providing limiting (limiter 384 of Fig. 11). Diode 624, resistor 626, and
capacitor 628 constitute the peak rectifier 386, 388 (Fig. 11), giving high amplitude
decaying pulses. Capacitor 630 and resistor 632 constitute the smoothing circuit 390
(Fig. 11). The feed to the low frequency fixed band circuit is taken through resistor
634 and diode 636. The feed to the low frequency sliding band circuit is taken through
resistor 638 and diode 640.
[0119] The low frequency overshoot circuit operates as a type of early warning circuit to
sense the buildup of signals. Reliance on the primary overshoot suppression circuit
alone would result in no overshoot suppression action until the threshold of the primary
overshoot suppression circuit is reached. The low frequency overshoot suppression
circuit highly amplifies to generate a vigorous pulse which is peak rectified and
held and fed through a high value resistor to gently charge the capacitor from which
the control circuit is derived. In operation, the circuit is useful in smoothing the
abrupt increases in the control signal caused by the primary overshoot suppression
circuit.
[0120] Figures 18 through 25 are examples of waveforms that are useful in describing the
operation of the overshoot suppression circuits. In Figures 18 through 22, the horizontal
axis is time and the vertical axis is voltage. Assume that the input signal to a stage
(for example, the high frequency high level stage) is as shown in Figure 18, namely
a sine wave signal (at 1 kHz, for example) that rises slowly from zero (the increase
is slow enough that the steady-state portions of the fixed band and sliding band control
circuits can follow the signal) up to a level of about - 25 dB (relative to the reference
level which is about 20 dB below the maximum level in the system). The threshold (the
onset of dynamic action, compression in this example) of the stage is assumed to be
-30 dB. After a sufficient period of time for the circuit to reach equilibrium (the
output signal amplitude stabilizes at some level), the input signal amplitude is suddenly
increased to -10 dB and kept at that level long enough for the circuit to reach equlibrium
once again.
[0121] Figure 19 depicts an example of how the fixed band or the sliding band control voltage
of the stage reacts to the input signal, with and without the primary overshoot circuit.
Figure 20 shows an example of the output of the primary overshoot circuit associated
with the fixed band or the sliding band portion of the stage in response to the input
signal. Figure 21 shows an example of the overall stage output without the use of
any overshoot suppression circuits and Figure 22 shows an example of the overall stage
output with the use of overshoot suppression circuits.
[0122] As the input signal rises from zero to -25 dB, the control signal voltage rises smoothly
to a stable value in response to the -25 dB input level. At the same time the output
of the overshoot suppression circuit (an amplitude scaled full-wave rectified version
of the input signal) rises. However, because the steady-state portion of the control
circuit is able to follow the input signal, the amplitude of the overshoot suppression
circuit is less that the output of the steady-state portion of the control circuit
(it has less gain) and thus the overshoot suppression circuit does not contribute
to the charging of the second smoothing circuit capacitor and to the control signal
voltage under these circumstances. In Figures 21 and 22, which are the same during
this period, the output signal slowly rises, but to a lower level than the input signal
because of the compression action of the stage.
[0123] When the input signal jumps to -10 dB, the overshoot suppression circuit output also
jumps immediately in amplitude because there is essentially no time delay in its circuit.
The only significant delay is caused by the slew rate of the operational amplifier
and the ability of the second integrating capacitor to charge instantaneously, resulting
in about a 10 microsecond delay which results in an overshoot of about that time length--so
short as to be essentially ultrasonic. Because of the time constants of the first
and second smoothing circuits, the steady-state portion of the control circuit is
unable to follow immediately the jump in the input signal amplitude. Thus, the charging
output of the overshoot suppression circuit is greater than the charging output of
the steady-state portion of the control circuit and the overshoot suppression circuit
is responsible for charging the second smoothing circuit capacitor until enough time
elapses for the steady-state portion of the control circuit to catch up. Figure 19
shows how the control voltage is "bumped up" by the overshoot suppression circuit
charging current shown in Figure 20. The portion of Figure 20 labeled "w/o O/S" (without
overshoot) indicates the manner in which the control voltage would slowly increase
in response only to the steady-portion of the control circuit, without any assistance
from the overshoot suppression side circuit.
[0124] Figure 21 shows how the output signal would rise to a very high level and then slowly
decay to the steady-state condition as the control signal without overshoot suppression
slowly rises to its equilibrium level, whereas Figure 22 shows the output signal rising
only briefly to a value only slightly higher than its equilibrium level as the overshoot
suppression circuit causes a quick, but controlled, increase in the control voltage.
[0125] Figure 23 shows in greater detail an example of the interrelationship between the
overshoot suppression charging current and the control voltage as a the input level
is suddenly increased from -25 dB to -10 dB. The Figure is an expanded view showing
only the first tens of milliseconds or so. Figure 24 is similar to Figure 23 but shows
the overshoot suppression charging current and the control voltage over a much longer
period of time, hundreds of milliseconds or so. The envelope of the overshoot suppression
circuit pulses decays to a steady-state level as the stage output reaches equilibrium
while at the same time the control voltage derived from the capacitor voltage slowly
increases in response to charging by the steady-state portion of the control circuit.
The overshoot suppression circuit acts only briefly to rapidly increase the capacitor
voltage to a level close to, but less than, its ultimate steady- state value.
[0126] It will be noted that the effect of the overshoot suppression circuit in these examples
is to cause some interruption in the smoothness of the control voltage. The extent
to which the control voltage smoothness is affected depends on the severity of the
change in the input signal. An important feature of the overshoot suppression circuit
is that its output is related to the rate of change of the input signal. This is accomplished
by operating the coupling diode 568 (Fig. 14) so that the diode is forward biased
into the knee of its operating curve as shown in Figure 25. The charging current thus
increases as the input voltage increases. Diode 566 and resistor 564 (Fig. 14) assist
in assuring that the circuit does not provide more charging current than required
by reducing the amplifier gain for higher level signals.
[0127] A basic feature of the interraction between the steady-state portion of the control
circuit and the overshoot suppression portion is that the combined arrangement acts
abruptly when it has to and as soon as it can it lets loose of the fast action and
moves into a slow acting regime. Consequently, most of the time the overshoot suppression
circuit is not acting at all. Most of the time the signal is controlled by well smoothed
control signals.
[0128] The secondary overshoot circuit (Fig. 17) operates in essentially the same way as
the primary overshoot circuit. The secondary overshoot suppression circuit is required
whenever a smoothed modulation control signal is used to provide the threshold tracking
effect in the primary overshoot suppression circuit because the smoothing filter destroys
the ability of the circuit to discriminate frequencies.
Appendix
Component Values for Figures 12-14, 16 & 17
[0129] (For resistors, xKy means x.y kilohms; xMy means x.y megohms; xyK means xy kilohms;
capacitors are in microfarads; diodes are silicon diodes)
Figure 12
[0130] For high level, high frequency, sliding band stage:
402 4K7
410 4K7
412 18K
414 36K
416 68K
420 0.1
422 82K
426 22K
428 750K
432 15K
434 1K5
436 220K
438 7M5
442 100 ohms
444 0.1
[0131] For high level, low frequency, sliding band stage:
402 3K6
410 3K6
412 12K
414 24K
416 30K
420 0.1
422 75K
426 22K
428 680K
432 15K
434 1K5
436 680K
438 6M8
442 100 ohms
444 0.22
[0132] For mid-level, high frequency, sliding band stage:
402 3K6
410 3K6
412 2K7
414 5K6
416 6K8
420 0.1
422 43K
426 22K
428 750K
432 15K
434 1K5
436 220K
438 7M5
442 100 ohms
444 0.1
[0133] For mid-level, low frequency, sliding band stage:
402 3K6
410 3K6
412 3K9
414 8K2
416 10K
420 0.1
422 75K
426 22K
428 680K
432 15K
434 2K2
436 680K
438 6M8
442 100 ohms
444 0.22
[0134] For low level, high frequency, sliding band stage:
402 3K3
410 3K3
412 2K7
414 2K2
416 2K7
420 0.1
422 33K
426 22K
428 750K
432 15K
434 1K5
436 220K
438 7M5
442 100 ohms
444 0.1
Figure 13
[0135] High level, high frequency, fixed band stage:
452 10K
460 10K
462 16K
464 33K
466 110K
470 0.1
472 82K
482 56K
490 15K
492 16K
494 33K
498 0.1
500 82K
502 3K9
504 1M6
512 100 ohms
514 0.1
[0136] High level, low frequency, fixed band stage:
452 9K1
460 9K1
462 62K
464 120K
466 200K
470 0.1
472 150K
482 22K
490 22K
492 51K
494 100K
498 0.1
500 150K
502 13K
504 1M3
512 100 ohms
514 0.22
[0137] Mid-level, high frequency, fixed band stage:
452 4K7
460 4K7
462 5K1
464 10K
466 36K
470 0.1
472 82K
482 8K2
490 8K2
492 5K1
494 10K
498 0.1
500 82K
502 3K9
504 1M6
512 100 ohms
514 0.1
[0138] Mid-level, low frequency, fixed band stage:
452 13K
460 13K
462 20K
464 39K
466 68K
470 0.1
472 150K
482 220K
490 220K
492 16K
494 33K
498 0.1
500 150K
502 13K
504 1M3
512 100 ohms
514 0.22
[0139] Low level, high frequency, fixed band stage:
452 4K7
460 4K7
462 2K7
464 5K6
466 18K
470 0.1
472 82K
482 3K3
490 3K3
492 2K7
494 5K6
498 0.1
500 82K
502 3K9
504 1M6
512 100 ohms
514 0.1
Figure 14
[0140] High level, high frequency, sliding band stage:
546 130K
548 68K
552 47K
558 62K
560 22K
562 1 megohm
564 22K
[0141] High level, high frequency, fixed band stage:
546 120K
548 62K
552 390K
558 62K
560 22K
562 1 megohm
564 15K
[0142] High level, low frequency, sliding band stage:
546 10K
548 5K1
552 MC5--82K; MC7--15K; MC8--3K3
558 68K
560 22K
562 1 megohm
564 15K
[0143] High level, low frequency, fixed band stage:
546 10K
548 5K1
552 MC7--15K; MC8--5K1
558 68K
560 22K
562 1 megohm
564 15K
[0144] Mid-level, high frequency, sliding band stage:
546 43K
548 22K
552 6K8
558 62K
560 22K
562 1 megohm
564 10K
[0145] Mid-level, high frequency, fixed band stage:
546 39K
548 20K
552 120K
558 62K
560 22K
562 1 megohm
564 1K5
[0146] Mid-level, low frequency, sliding band stage:
546 3K3
548 1K6
552 MC5--27K; MC7--4K7; MC8--6K8
558 63K
560 22K
562 1 megohm
564 15K
[0147] Mid-level, low frequency, fixed band stage:
546 3K3
548 1K6
552 MC7--4K7; MC8--6K8
558 68K
560 22K
562 1 megohm
564 6K8
[0148] Low level, high frequency, sliding band stage:
546 22K
548 11K
552 3K3
558 62K
560 22K
562 1 megohm
564 10K
[0149] Low level, high frequency, fixed band stage:
546 20K
548 10K
552 62K
558 62K
560 22K
562 1 megohm
564 1K5
Figure 16
[0151] High level, low frequency, fixed band stage:
580 150K
582 75K
584 300K
590 150K
592 2K2
596 40K
600 1K
602 47K
[0152] Mid-level, low frequency, fixed band stage:
580 47K
582 24K
584 100K
590 47K
592 2K2
596 40K
600 1K
602 47K
Figure 17
[0153] High level, low frequency, fixed band stage:
610 62K
612 30K
614 150K
616 6K8
618 620K
622 680K
626 47K
628 0.47
630 0.1
632 470K
634 470K
638 1 megohm
[0154] Mid-level, low frequency, fixed band stage:
610 30K
612 15K
614 47K
616 10K
618 910K
622 1 megohm
626 47K
628 0.47
630 0.1
632 47K
634 680K
638 820K
1. A circuit for modifying the dynamic range of an input signal, comprising
means for modifying the dynamic range of said input signal in response to a control
signal to provide an output signal, and
means for generating said control signal, said means including
capacitance means,
means for charging said capacitance means with a first signal derived from said output
signal, said first signal varying more slowly than said output signal,
means for charging said capacitance means with a second signal derived from said output
signal, said second signal varying substantially as quickly as said output signal,
and
means for deriving said control signal from the charge on said capacitance means.
2. The circuit of claim 1 wherein said means for charging the capacitance means with
a first signal comprises means in a first signal path and said means for charging
the capacitance means with a second signal comprises means in a second signal path.
3. The circuit of claim 2 wherein the steepness of the variation of said second signal
changes with the rate of change of variation in said output signal.
4. The circuit of claims 1, 2, or 3 wherein said means for charging the capacitance
means with a second signal charges said capacitance means to a level substantially
no greater than the level to which the means for charging the capacitance means with
a first signal later charges the capacitance means in response to the same portion
of the output signal.
5. The circuit of claim 4 wherein said means for generating said control signal further
comprises means for charging said capacitance means with a third signal derived from
said output signal, said third signal responding to low frequency increases in the
amplitude of said output signal.
6. The circuit of claims 1, 2, or 3 wherein said first signal has a charging effect
larger than the charging effect of said second signal for slowly changing input signals
and the second signal has a charging effect larger than the charging effect of said
first signal means for rapidly changing input signals.
7. The circuit of claim 6 wherein said means for generating said control signal further
comprises means for charging said capacitance means with a third signal derived from
said output signal, said third signal responding to low frequency increases in the
amplitude of said output signal.
8. A circuit for modifying the dynamic range of an input signal, comprising
means for modifying the dynamic range of said input signal in response to a control
signal to provide an output signal, and
means for generating said control signal, said means including
means for deriving a first signal from said output signal,
means for rectifying said first signal,
means, including capacitance means, for smoothing the rectified first signal,
means for deriving a second signal from said output signal,
means for rectifying said second signal,
diode means, and
means for coupling the rectified second signal to said capacitance means via said
diode means, and
means for deriving said control signal from the charge on said capacitance means.
9. The circuit of claim 8 wherein said means for deriving said first signal, said
means for rectifying said first signal, and said means for smoothing said rectified
first signal comprise a steady-state signal path and wherein said means for deriving
said second signal, said means for rectifying said second signal, said diode means,
and said means for coupling said rectified second signal to said capacitance means
via said diode means comprise an overshoot suppression signal path.
10. The circuit of claim 9 wherein said overshoot suppression signal path has a time
constant for charging said capacitance means substantially shorter than the time constant
of the steady-state signal path for charging said capacitance means, whereby transient
input signal components are rapidly applied to said capacitance means via said overshoot
suppression signal path.
11. The circuit of claims 8 or 9 wherein the gain of said overshoot suppression signal
path is less than the gain of the steady-state signal path, whereby the overshoot
suppression signal path charges said capacitance means to a level substantially no
greater that the level to which the steady-state signal path charges the capacitance
means in response to the same portion of the output signal.
12. The circuit of claim 11 wherein said means for coupling the rectified second signal
to said capacitance means via said diode means includes means for operating said diode
means in that portion of its diode characteristic such that said diode means exhibits
the variable current characteristics.
13. The circuit of claim 12 further comprising
means for deriving a third signal from said output signal, said third signal responding
to low frequency increases in the amplitude of said output signal,
additional diode means, and
means for coupling said third signal to said capacitance means via said additional
diode means.
14. The circuit of claim 8 wherein said means for smoothing the rectified first signal
includes a first smoothing stage and a second smoothing stage, said second smoothing
stage including said capacitance means and said first smoothing stage including further
capacitance means, said first smoothing stage having a shorter attack time constant
than said second smoothing stage.
15. A circuit for modifying the dynamic range of an input signal, comprising
frequency selective circuit means for dividing the frequency spectrum in which the
input signal lies into pass-band and stop-band regions,
means for modifying the dynamic range of signal components in the pass-band region
in response to a control signal to provide an output signal, said control signal acting
in response to signal components lying in the pass-band and stop-band regions,
means for deriving at least one modulation control signal from said output signal,
said modulation control signal having the characteristic that when combined in opposition
with said control signal, the control signal is altered, in a level dependent way,
so as to make the control signal less responsive to stop-band signal components as
the level of the input signal rises, and
means for generating said control signal, said means including
means for deriving a first signal from said output signal,
means for rectifying said first signal,
means for combining a modulation control signal in opposition with the rectified first
signal,
means, including capacitance means, for smoothing the rectified first signal combined
in opposition with a modulation control signal,
means for deriving a second signal from said output signal,
means for rectifying said second signal,
means for combining a modulation control signal in opposition with the rectified second
signal,
diode means,
means for coupling the rectified second signal combined in opposition with a modulation
control signal to said capacitance means via said diode means, and
means for deriving said control signal from the charge on said capacitance means.
16. The circuit of claim 15 wherein the same modulation control signal is combined
in opposition to said first and second signals.
17. The circuit of claim 15 wherein the modulation control signal combined in opposition
to said second signal is a smoothed version of the modulation control signal combined
in opposition to said first signal.
18. The circuit of claim 15 wherein said means for smoothing the rectified first signal
includes a first smoothing stage and a second smoothing stage, said second smoothing
stage including said capacitance means and said first smoothing stage including further
capacitance means, said first smoothing stage having a shorter attack time constant
than said second smoothing stage.
19. Three circuits in accordance with claim 15 arranged in series, wherein said at
least one modulation control signal for use in all three circuits is derived from
the output of the second circuit.
20. The circuit of claim 15 wherein said means for deriving said first signal, said
means for rectifying said first signal, said means for combining a modulation control
signal in opposition with the rectified first signal, and said means for smoothing
said rectified first signal combined with a modulation control signal comprise a steady-state
signal path and wherein said means for deriving said second signal, said means for
rectifying said second signal, said means for combining a modulation control signal
in opposition with the rectified second signal, said diode means, and said means for
coupling said second signal to said capacitance means via said diode means comprise
an overshoot suppression signal path.
21. The circuit of claim 20 wherein said overshoot suppression signal path has a time
constant for charging said capacitance means substantially shorter than the time constant
of the steady-state signal path for charging said capacitance means, whereby transient
input signal components are rapidly applied to said capacitance means via said overshoot
suppression signal path.
22. The circuit of claims 20 or 21 wherein the gain of said overshoot suppression
signal path is less than the gain of the steady-state signal path, whereby the overshoot
suppression signal path charges said capacitance means to a level substantially no
greater thatn the level to which the steady-state signal path charges the capacitance
means in response to the same portion of the output signal.
23. The circuit of claim 22 wherein said means for coupling the rectified second signal
to said capacitance means via said diode means includes means for operating said diode
means in that portion of its diode characteristic such that said diode means exhibits
the variable current characteristics.
24. The circuit of claim 23 further comprising
means for deriving a third signal from said output signal, said third signal responding
to low frequency increases in the amplitude of said output signal,
means for combining a modulation control signal in opposition to said third signal,
additional diode means, and
means for coupling said third signal to said capacitance means via said additional
diode means.
25. A circuit for modifying the dynamic range of an input signal, comprising
first dynamic action means having a fixed band characteristic action acting in response
to a first control signal to provide a first output signal, said first dynamic action
means including means for generating a first control signal, said means for generating
a first control signal including
means for deriving a first signal from said first output signal,
means for rectifying said first signal,
means, including capacitance means, for smoothing the rectified first signal,
means for deriving a second signal from said first output signal,
means for rectifying said second signal,
first diode means, and
means for coupling the rectified second signal to said capacitance means via said
first diode means, and
means for deriving said first control signal from the charge on said capacitance means,
second dynamic action means having a sliding band characteristic action in response
to a second control signal to provide a second output signal, said second dynamic
action means including means for generating a second control signal, said means for
generating a second control signal including
means for deriving a third signal from said second output signal,
means for rectifying said third signal,
means, including further capacitance means, for smoothing the rectified third signal,
means for deriving a fourth signal from said output signal,
means for rectifying said fourth signal,
second diode means,
means for coupling the rectified fourth signal to said further capacitance means via
said second diode means, and
means for deriving said control signal from the charge on said capacitance means,
and
means for coupling said first dynamic action means to said second dynamic action means.
26. The circuit of claim 25 wherein said means for generating a first control signal
further comprises means, including third diode means, for charging said capacitance
means with a fifth signal derived from said first output signal, said fifth signal
responding to low frequency increases in the amplitude of said first output signal
and wherein said means for generating a second control signal further comprises means,
including fourth diode means, for charging said further capacitance means with said
fifth signal.
27. The circuit of claim 25 wherein said means for generating a second control signal
further comprises means for charging said further capacitance means with said second
signal.
28. The circuit of claims 25 or 26 further comprising
means for deriving a sixth signal from said first output signal,
means for rectifying said sixth signal, sixth diode means, and
means for coupling the rectified sixth signal to said capacitance means via said sixth
diode means.
29. The circuit of claim 28 further comprising
seventh diode means, and
means for coupling the rectified sixth signal to said further capacitance means via
said seventh diode means.
30. The circuit of claim 28 wherein said means for generating a first control signal
further comprises means, including third diode means, for charging said capacitance
means with a fifth signal derived from said first output signal, said fifth signal
responding to low frequency increases in the amplitude of said first output signal
and wherein said means for generating a second control signal further comprises means,
including fourth diode means, for charging said further capacitance means with said
fifth signal.
31. The circuit of claim 29 wherein said means for generating a first control signal
further comprises means, including third diode means, for charging said capacitance
means with a fifth signal derived from said first output signal, said fifth signal
responding to low frequency increases in the amplitude of said first output signal
and wherein said means for generating a second control signal further comprises means,
including fourth diode means, for charging said further capacitance means with said
fifth signal.
32. A circuit for modifying the dynamic range of an input signal, comprising
means for modifying the dynamic range of said input signal in response to a control
signal to provide an output signal, and
means for generating said control signal, said means including capacitance means from
which the control signal is derived, and
said means for generating said control signal further comprising means for charging
said capacitance means with a signal derived from said output signal, said signal
responding to low frequency increases in the amplitude of said output signal.
33. The circuit of claim 8 wherein said means for rectifying said first signal does
not include a peak rectifier.
34. The circuit of claim 15 wherein said means for rectifying said first signal does
not include a peak rectifier.
35. The circuit of claim 25 wherein said means for rectifying said first signal does
not include a peak rectifier.